Advanced Neutron Sources 1988, Proceedings of the 10th Meeting of the INT Collaboration on Advanced Neutron Sources (ICANS X), Held at Los Alamos, October 1988Revolving around the interaction between spectrometer and target-station design and performance, this volume emphasises the need for feedback that must exist between scientific requirements and source design. It achieves a forum for the sharing of information on the development of spallation neutron sources. Of great value to researchers in condensed matter physics, instrumentation and data processing involved in neutron scattering at pulsed and steady sources. |
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Page 206
... geometry , cold - source geometry , and coupling surfaces . To simplify the calculations as much as possible , they will be carried out in a two - dimensional r - z geometry . In Fig . 1 two cylindrical geometries - the reactor geometry ...
... geometry , cold - source geometry , and coupling surfaces . To simplify the calculations as much as possible , they will be carried out in a two - dimensional r - z geometry . In Fig . 1 two cylindrical geometries - the reactor geometry ...
Page 207
... geometry , azimuthal symmetry is assumed ; this symmetry does not exist in the reactor geometry . To test the validity of these approximations , the thermal neutron flux , as a function of distance along the cold - source z - axis as ...
... geometry , azimuthal symmetry is assumed ; this symmetry does not exist in the reactor geometry . To test the validity of these approximations , the thermal neutron flux , as a function of distance along the cold - source z - axis as ...
Page 234
... geometry is simple since it is a straightforward transmission experiment and the angular structure of the detector need not be dealt with in data collection . The transmission geometry also allows the collection of position - sensitive ...
... geometry is simple since it is a straightforward transmission experiment and the angular structure of the detector need not be dealt with in data collection . The transmission geometry also allows the collection of position - sensitive ...
Contents
Monday October 3 1988 | 9 |
Tuesday October 4 1988 | 135 |
Wednesday October 5 1988 | 609 |
Copyright | |
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accelerator Advanced Neutron Sources analysis angular background beam line Brillouin scattering calculated chopper cold neutron cold source collimators count rate cross section crystal data acquisition deconvolution decoupled density detector deuterium diffraction diffractometer distribution dose effective energy transfer experimental experiments facility factor Figure fission flight path foil function gamma Gaussian geometry high-energy histogram improve increase inelastic injection instrument intensity IPNS ISIS LAMPF leakage liquid hydrogen Los Alamos magnetic material MaxEnt maximum measured methane module Monte Carlo neutron beam neutron flux neutron scattering Nucl Nuclear obtained operation optimization parameters peak performance Phys position present problems produced proton proton beam radiation radius range reactor reconstruction reflector resolution Rutherford Appleton Laboratory sample scattering angle shield shown in Fig shows solid methane spallation neutron source spallation source spectra spectrometer spectrum surface temperature thermal neutron thick time-of-flight tube wavelength width